How Does Coulomb's Law and Vectors Determine the Direction of Force?

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SUMMARY

Coulomb's Law defines the force between two charges as F = k * (q1 * q2) / r12^2 * (r12)/r12, where r12 is the vector distance between the charges. The direction of the force is determined by the signs of the charges: if q1 and q2 have the same sign, the force is repulsive, and if they have opposite signs, the force is attractive. The unit vector, denoted as &hat;r12, indicates the direction of the force, pointing away from the source charge for like charges and towards the source charge for unlike charges. Understanding this vector relationship is crucial for correctly applying Coulomb's Law in electrostatics.

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bifodus
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To find the magnitude of a force between two charges is very simple, but to get the direction of the force seems a little strange to me. The signs of the charges aren't included anywhere in the law, so does this mean that I literally have to think "the signs are opposite, therefore I will multiply the vector by -1 (or leave it positive, depending on my reference coordinates)"? This seems a little bit cumbersome and forced to me, and apparently not derived anywhere in the mathematics of it. Am I going about doing this the right way?

I'm quite accustomed with vectors (vector calculus and linear algebra background), but very new to e&m. Any help would be much appreciated.
 
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The signs are included in Coulomb's law.
 
"The signs of the charges are not included anywhere in the law". Hmmmmmmmmmmm.
I have a good book with an equation that should help you out.

F= C q1 q2 / r12^2 * (r12)/r12

Where the bolds are vectors, the regular font is scalar
and r12 =r1-r2
where r1 is the location of the q1 and
r2 is the location of q2

If I'm not too clear, I'll fix it up some more
 
The "force on q1 due to q2" is (in agreement with sinyud)
\vec F_{on\ q_1\ due\ to\ q_2} = k\frac{q_1 q_2}{r_{12}{}^2} \hat r_{12}
where \hat r_{12} is the unit vector at the target charge q_1 pointing away from the source charge q_2 and
r_{12} is the distance to the target charge q_1 from the source charge q_2.

If the product q_1q_2 is positive (so they have like signs), then,
since \hat r_{12} points away from q_2, it follows that\vec F_{on\ q_1\ due\ to\ q_2} points away from q_2.
"q_1 is repelled by q_2."

If the product q_1q_2 is negative (so they have unlike signs), then,
since \hat r_{12} points away from q_2, it follows that \vec F_{on\ q_1\ due\ to\ q_2} points towards q_2.
"q_1 is attracted to q_2."
 
Ahh, thanks guys. For some reason I was attaching the unit vector to the equation for the magnitude of the force, which obviously removes the signs from the charges. Major brain fart.

Thanks again.
 

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